It is interesting to note that the recent analysis of the \(B^+\rightarrow J/\psi \phi K^+\) 
process [1]}, and the study of the masses of \(cs\bar{cs}\)  tetraquark
states [2]} seem to favor that the \(X(4274)\)  may be the conventional \(\chi _{c1}(3P)\)  state.
If \(X(4274)\)  is assigned as the \(\chi _{c1}(3P)\)  state, then one
immediate question is how to understand \(X(4140)\) . In Ref. [1]} the analysis suggests that the \(X(4140)\)  structure
may not be a genuine resonance. There are possibilities for a non-resonance interpretation for \(Y(4140)\) , such as the \(D_sD_s^*\)  CUSP [4]}, [5]}, or \(D_sD_s^*\)  rescatterings via the open-charmed meson loops [1]}.
To better understand \(X(4140)\)  and \(X(4274)\) , experimental studies of their open-charm decay modes,
i.e. \(DD^*\) , \(D^*D^*\)  and \(D_sD^*_s\) , are strongly recommended.
